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	<title>RESONEUT - Revision history</title>
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	<updated>2026-04-12T21:33:35Z</updated>
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	<entry>
		<id>https://fsunuc.physics.fsu.edu/wiki/index.php?title=RESONEUT&amp;diff=2070&amp;oldid=prev</id>
		<title>Rtang at 01:13, 25 October 2023</title>
		<link rel="alternate" type="text/html" href="https://fsunuc.physics.fsu.edu/wiki/index.php?title=RESONEUT&amp;diff=2070&amp;oldid=prev"/>
		<updated>2023-10-25T01:13:35Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
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				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;Revision as of 21:13, 24 October 2023&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l1&quot;&gt;Line 1:&lt;/td&gt;
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&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;[[File:Schematic cross-section of RESONEUT.png|thumb|right|Schematic cross-section of RESONEUT&amp;lt;ref name=&amp;quot;NIMA&amp;quot; /&amp;gt;]]&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;[[File:Schematic cross-section of RESONEUT.png|thumb|right|Schematic cross-section of RESONEUT&amp;lt;ref name=&amp;quot;NIMA&amp;quot; /&amp;gt;]]&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br/&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br/&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;RESONEUT &amp;lt;ref name=&amp;quot;NIMA&amp;quot;&amp;gt; L. T. Baby, S. A. Kuvin, I. Wiedenhover &amp;#039;&amp;#039;et al.&amp;#039;&amp;#039;, Nulc. Inst. Meth. Phys. A, &amp;#039;&amp;#039;&amp;#039;877&amp;#039;&amp;#039;&amp;#039;, 34 (2018) https://doi.org/10.1016/j.nima.2017.09.019 &amp;lt;/ref&amp;gt; is built for spectroscopy of low-lying proton resonances using (d,n) reactions in inverse kinematics with radioactive beams. The setup consists of 9 &amp;#039;&amp;#039;&amp;#039;p-terphenyl&amp;#039;&amp;#039;&amp;#039; scintillator crystals as neutron detectors placed 23 cm upstream of the target, along with silicon strip detectors, a gas ionization chamber, and NaI detectors. The p-terphenyl crystals provide good detection efficiency for low-energy neutrons below 300 keV emitted at backward angles in the reactions of interest. Pulse shape discrimination is used to distinguish neutrons from gamma background. Experiments were performed with stable &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;12C &lt;/del&gt;beams on deuterated targets, populating proton resonances in &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;13N&lt;/del&gt;. The setup achieved ~200 keV energy resolution, a detection efficiency of around 0.5% per crystal, and a total efficiency of around 2-5% depending on neutron energy. Overall this provides a compact, high-efficiency system to study low-lying resonances with radioactive beams using (d,n) reactions.&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;RESONEUT &amp;lt;ref name=&amp;quot;NIMA&amp;quot;&amp;gt; L. T. Baby, S. A. Kuvin, I. Wiedenhover &amp;#039;&amp;#039;et al.&amp;#039;&amp;#039;, Nulc. Inst. Meth. Phys. A, &amp;#039;&amp;#039;&amp;#039;877&amp;#039;&amp;#039;&amp;#039;, 34 (2018) https://doi.org/10.1016/j.nima.2017.09.019 &amp;lt;/ref&amp;gt; is built for spectroscopy of low-lying proton resonances using (d,n) reactions in inverse kinematics with radioactive beams. The setup consists of 9 &amp;#039;&amp;#039;&amp;#039;p-terphenyl&amp;#039;&amp;#039;&amp;#039; scintillator crystals as neutron detectors placed 23 cm upstream of the target, along with silicon strip detectors, a gas ionization chamber, and NaI detectors. The p-terphenyl crystals provide good detection efficiency for low-energy neutrons below 300 keV emitted at backward angles in the reactions of interest. Pulse shape discrimination is used to distinguish neutrons from gamma background. Experiments were performed with stable &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&amp;lt;sup&amp;gt;12&amp;lt;/sup&amp;gt;C &lt;/ins&gt;beams on deuterated targets, populating proton resonances in &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&amp;lt;sup&amp;gt;13&amp;lt;/sup&amp;gt;N&lt;/ins&gt;. The setup achieved &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&amp;#039;&amp;#039;&amp;#039;&lt;/ins&gt;~200 keV energy resolution&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&amp;#039;&amp;#039;&amp;#039;&lt;/ins&gt;, a detection efficiency of around &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&amp;#039;&amp;#039;&amp;#039;&lt;/ins&gt;0.5% per crystal&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&amp;#039;&amp;#039;&amp;#039;&lt;/ins&gt;, and a total efficiency of around 2-5% depending on neutron energy. Overall this provides a compact, high-efficiency system to study low-lying resonances with radioactive beams using (d,n) reactions.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;

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		<author><name>Rtang</name></author>
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	<entry>
		<id>https://fsunuc.physics.fsu.edu/wiki/index.php?title=RESONEUT&amp;diff=2069&amp;oldid=prev</id>
		<title>Rtang at 01:11, 25 October 2023</title>
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		<updated>2023-10-25T01:11:33Z</updated>

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				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;Revision as of 21:11, 24 October 2023&lt;/td&gt;
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&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;[[File:Schematic cross-section of RESONEUT.png|thumb|right|Schematic cross-section of RESONEUT &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;(Take from &lt;/del&gt;NIMA&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;, 877 (2018) 34 )&lt;/del&gt;]]&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;[[File:Schematic cross-section of RESONEUT.png|thumb|right|Schematic cross-section of RESONEUT&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&amp;lt;ref name=&amp;quot;&lt;/ins&gt;NIMA&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&amp;quot; /&amp;gt;&lt;/ins&gt;]]&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br/&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br/&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;RESONEUT &amp;lt;ref&amp;gt; L. T. Baby, S. A. Kuvin, I. Wiedenhover &amp;#039;&amp;#039;et al.&amp;#039;&amp;#039;, Nulc. Inst. Meth. Phys. A, &amp;#039;&amp;#039;&amp;#039;877&amp;#039;&amp;#039;&amp;#039;, 34 (2018) https://doi.org/10.1016/j.nima.2017.09.019 &amp;lt;/ref&amp;gt; is built for spectroscopy of low-lying proton resonances using (d,n) reactions in inverse kinematics with radioactive beams. The setup consists of 9 &amp;#039;&amp;#039;&amp;#039;p-terphenyl&amp;#039;&amp;#039;&amp;#039; scintillator crystals as neutron detectors placed 23 cm upstream of the target, along with silicon strip detectors, a gas ionization chamber, and NaI detectors. The p-terphenyl crystals provide good detection efficiency for low-energy neutrons below 300 keV emitted at backward angles in the reactions of interest. Pulse shape discrimination is used to distinguish neutrons from gamma background. Experiments were performed with stable 12C beams on deuterated targets, populating proton resonances in 13N. The setup achieved ~200 keV energy resolution, a detection efficiency of around 0.5% per crystal, and a total efficiency of around 2-5% depending on neutron energy. Overall this provides a compact, high-efficiency system to study low-lying resonances with radioactive beams using (d,n) reactions.&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;RESONEUT &amp;lt;ref &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;name=&amp;quot;NIMA&amp;quot;&lt;/ins&gt;&amp;gt; L. T. Baby, S. A. Kuvin, I. Wiedenhover &amp;#039;&amp;#039;et al.&amp;#039;&amp;#039;, Nulc. Inst. Meth. Phys. A, &amp;#039;&amp;#039;&amp;#039;877&amp;#039;&amp;#039;&amp;#039;, 34 (2018) https://doi.org/10.1016/j.nima.2017.09.019 &amp;lt;/ref&amp;gt; is built for spectroscopy of low-lying proton resonances using (d,n) reactions in inverse kinematics with radioactive beams. The setup consists of 9 &amp;#039;&amp;#039;&amp;#039;p-terphenyl&amp;#039;&amp;#039;&amp;#039; scintillator crystals as neutron detectors placed 23 cm upstream of the target, along with silicon strip detectors, a gas ionization chamber, and NaI detectors. The p-terphenyl crystals provide good detection efficiency for low-energy neutrons below 300 keV emitted at backward angles in the reactions of interest. Pulse shape discrimination is used to distinguish neutrons from gamma background. Experiments were performed with stable 12C beams on deuterated targets, populating proton resonances in 13N. The setup achieved ~200 keV energy resolution, a detection efficiency of around 0.5% per crystal, and a total efficiency of around 2-5% depending on neutron energy. Overall this provides a compact, high-efficiency system to study low-lying resonances with radioactive beams using (d,n) reactions.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;

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	<entry>
		<id>https://fsunuc.physics.fsu.edu/wiki/index.php?title=RESONEUT&amp;diff=2068&amp;oldid=prev</id>
		<title>Rtang at 01:09, 25 October 2023</title>
		<link rel="alternate" type="text/html" href="https://fsunuc.physics.fsu.edu/wiki/index.php?title=RESONEUT&amp;diff=2068&amp;oldid=prev"/>
		<updated>2023-10-25T01:09:59Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;table style=&quot;background-color: #fff; color: #202122;&quot; data-mw=&quot;interface&quot;&gt;
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				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;Revision as of 21:09, 24 October 2023&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l1&quot;&gt;Line 1:&lt;/td&gt;
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&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;RESONEUT &amp;lt;ref&amp;gt; L. T. Baby, S. A. Kuvin, I. Wiedenhover &amp;#039;&amp;#039;et al.&amp;#039;&amp;#039;, Nulc. Inst. Meth. Phys. A, &amp;#039;&amp;#039;&amp;#039;877&amp;#039;&amp;#039;&amp;#039;, 34 (2018) &amp;lt;/ref&amp;gt; is built for spectroscopy of low-lying proton resonances using (d,n) reactions in inverse kinematics with radioactive beams. The setup consists of 9 p-terphenyl scintillator crystals as neutron detectors placed 23 cm upstream of the target, along with silicon strip detectors, a gas ionization chamber, and NaI detectors. The p-terphenyl crystals provide good detection efficiency for low-energy neutrons below 300 keV emitted at backward angles in the reactions of interest. Pulse shape discrimination is used to distinguish neutrons from gamma background. Experiments were performed with stable 12C beams on deuterated targets, populating proton resonances in 13N. The setup achieved ~200 keV energy resolution, a detection efficiency of around 0.5% per crystal, and a total efficiency of around 2-5% depending on neutron energy. Overall this provides a compact, high-efficiency system to study low-lying resonances with radioactive beams using (d,n) reactions.&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[[File:Schematic cross-section of RESONEUT.png|thumb|right|Schematic cross-section of RESONEUT (Take from NIMA, 877 (2018) 34 )]]&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-deleted&quot;&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt; &lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-deleted&quot;&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;RESONEUT &amp;lt;ref&amp;gt; L. T. Baby, S. A. Kuvin, I. Wiedenhover &amp;#039;&amp;#039;et al.&amp;#039;&amp;#039;, Nulc. Inst. Meth. Phys. A, &amp;#039;&amp;#039;&amp;#039;877&amp;#039;&amp;#039;&amp;#039;, 34 (2018) &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;https://doi.org/10.1016/j.nima.2017.09.019 &lt;/ins&gt;&amp;lt;/ref&amp;gt; is built for spectroscopy of low-lying proton resonances using (d,n) reactions in inverse kinematics with radioactive beams. The setup consists of 9 &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&amp;#039;&amp;#039;&amp;#039;&lt;/ins&gt;p-terphenyl&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&amp;#039;&amp;#039;&amp;#039; &lt;/ins&gt;scintillator crystals as neutron detectors placed 23 cm upstream of the target, along with silicon strip detectors, a gas ionization chamber, and NaI detectors. The p-terphenyl crystals provide good detection efficiency for low-energy neutrons below 300 keV emitted at backward angles in the reactions of interest. Pulse shape discrimination is used to distinguish neutrons from gamma background. Experiments were performed with stable 12C beams on deuterated targets, populating proton resonances in 13N. The setup achieved ~200 keV energy resolution, a detection efficiency of around 0.5% per crystal, and a total efficiency of around 2-5% depending on neutron energy. Overall this provides a compact, high-efficiency system to study low-lying resonances with radioactive beams using (d,n) reactions.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;

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		<id>https://fsunuc.physics.fsu.edu/wiki/index.php?title=RESONEUT&amp;diff=2066&amp;oldid=prev</id>
		<title>Rtang at 01:05, 25 October 2023</title>
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		<updated>2023-10-25T01:05:18Z</updated>

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				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;Revision as of 21:05, 24 October 2023&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l1&quot;&gt;Line 1:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 1:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;RESONEUT &amp;lt;ref&amp;gt; L. T. Baby &amp;lt;/ref&amp;gt; is built for spectroscopy of low-lying proton resonances using (d,n) reactions in inverse kinematics with radioactive beams. The setup consists of 9 p-terphenyl scintillator crystals as neutron detectors placed 23 cm upstream of the target, along with silicon strip detectors, a gas ionization chamber, and NaI detectors. The p-terphenyl crystals provide good detection efficiency for low-energy neutrons below 300 keV emitted at backward angles in the reactions of interest. Pulse shape discrimination is used to distinguish neutrons from gamma background. Experiments were performed with stable 12C beams on deuterated targets, populating proton resonances in 13N. The setup achieved ~200 keV energy resolution, a detection efficiency of around 0.5% per crystal, and a total efficiency of around 2-5% depending on neutron energy. Overall this provides a compact, high-efficiency system to study low-lying resonances with radioactive beams using (d,n) reactions.&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;RESONEUT &amp;lt;ref&amp;gt; L. T. Baby&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;, S. A. Kuvin, I. Wiedenhover &amp;#039;&amp;#039;et al.&amp;#039;&amp;#039;, Nulc. Inst. Meth. Phys. A, &amp;#039;&amp;#039;&amp;#039;877&amp;#039;&amp;#039;&amp;#039;, 34 (2018) &lt;/ins&gt;&amp;lt;/ref&amp;gt; is built for spectroscopy of low-lying proton resonances using (d,n) reactions in inverse kinematics with radioactive beams. The setup consists of 9 p-terphenyl scintillator crystals as neutron detectors placed 23 cm upstream of the target, along with silicon strip detectors, a gas ionization chamber, and NaI detectors. The p-terphenyl crystals provide good detection efficiency for low-energy neutrons below 300 keV emitted at backward angles in the reactions of interest. Pulse shape discrimination is used to distinguish neutrons from gamma background. Experiments were performed with stable 12C beams on deuterated targets, populating proton resonances in 13N. The setup achieved ~200 keV energy resolution, a detection efficiency of around 0.5% per crystal, and a total efficiency of around 2-5% depending on neutron energy. Overall this provides a compact, high-efficiency system to study low-lying resonances with radioactive beams using (d,n) reactions.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;

&lt;!-- diff cache key my_wiki:diff::1.12:old-2065:rev-2066 --&gt;
&lt;/table&gt;</summary>
		<author><name>Rtang</name></author>
	</entry>
	<entry>
		<id>https://fsunuc.physics.fsu.edu/wiki/index.php?title=RESONEUT&amp;diff=2065&amp;oldid=prev</id>
		<title>Rtang: Created page with &quot;RESONEUT &lt;ref&gt; L. T. Baby &lt;/ref&gt; is built for spectroscopy of low-lying proton resonances using (d,n) reactions in inverse kinematics with radioactive beams. The setup consists of 9 p-terphenyl scintillator crystals as neutron detectors placed 23 cm upstream of the target, along with silicon strip detectors, a gas ionization chamber, and NaI detectors. The p-terphenyl crystals provide good detection efficiency for low-energy neutrons below 300 keV emitted at backward ang...&quot;</title>
		<link rel="alternate" type="text/html" href="https://fsunuc.physics.fsu.edu/wiki/index.php?title=RESONEUT&amp;diff=2065&amp;oldid=prev"/>
		<updated>2023-10-25T01:03:30Z</updated>

		<summary type="html">&lt;p&gt;Created page with &amp;quot;RESONEUT &amp;lt;ref&amp;gt; L. T. Baby &amp;lt;/ref&amp;gt; is built for spectroscopy of low-lying proton resonances using (d,n) reactions in inverse kinematics with radioactive beams. The setup consists of 9 p-terphenyl scintillator crystals as neutron detectors placed 23 cm upstream of the target, along with silicon strip detectors, a gas ionization chamber, and NaI detectors. The p-terphenyl crystals provide good detection efficiency for low-energy neutrons below 300 keV emitted at backward ang...&amp;quot;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;RESONEUT &amp;lt;ref&amp;gt; L. T. Baby &amp;lt;/ref&amp;gt; is built for spectroscopy of low-lying proton resonances using (d,n) reactions in inverse kinematics with radioactive beams. The setup consists of 9 p-terphenyl scintillator crystals as neutron detectors placed 23 cm upstream of the target, along with silicon strip detectors, a gas ionization chamber, and NaI detectors. The p-terphenyl crystals provide good detection efficiency for low-energy neutrons below 300 keV emitted at backward angles in the reactions of interest. Pulse shape discrimination is used to distinguish neutrons from gamma background. Experiments were performed with stable 12C beams on deuterated targets, populating proton resonances in 13N. The setup achieved ~200 keV energy resolution, a detection efficiency of around 0.5% per crystal, and a total efficiency of around 2-5% depending on neutron energy. Overall this provides a compact, high-efficiency system to study low-lying resonances with radioactive beams using (d,n) reactions.&lt;/div&gt;</summary>
		<author><name>Rtang</name></author>
	</entry>
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